Flap opening dynamics in HIV-1 protease explored with a coarse-grained model

We present a one-bead coarse-grained model that enables dynamical simulations of proteins on the time scale of tens of microseconds. The parameterization of the force field includes accurate conformational terms that allow for fast and reliable exploration of the configurational space. The model is applied to the dynamics of flap opening in HIV-1 protease. The experimental structure of the recently crystallized semi-open conformation of HIV-1 protease is well reproduced in the simulation, which supports the accuracy of our model. Thanks to very long simulations and extensive sampling of opening and closing events, we also investigate the thermodynamics and kinetics of the opening process. We have shown that the effect of the solvent slows down the dynamics to the experimentally observed time scales. The model is found to be reliable for application to substrate docking simulations, which are currently in progress.     

Comparative analysis of the sequences and structures of HIV-1 and HIV-2 proteases

The different isolates available for HIV-1 and HIV-2 were compared for the region of the protease (PR) sequence, and the variations in amino acids were analyzed with respect to the crystal structure of HIV-1 PR with inhibitor. Based on the extensive homology (39 identical out of 99 residues), models were built of the HIV-2 PR complexed with two different aspartic protease inhibitors, acetylpepstatin and a renin inhibitor, H-261. Comparison of the HIV-1 PR crystal structure and the HIV-2 PR model structure and the analysis of the changes found in different isolates showed that correlated substitutions occur in the hydrophobic interior of the molecule and at surface residues involved in ionic or hydrogen bond interactions. The substrate binding residues of HIV-1 and HIV-2 PRs show conservative substitutions of four residues. The difference in affinity of HIV-1 and HIV-2 PRs for the two inhibitors appears to be due in part to the change of Val 32 in HIV-1 PR to Ile in HIV-2 PR.     

Structural insights into the South African HIV-1 subtype C protease: impact of hinge region dynamics and flap flexibility in drug resistance

The HIV protease plays a major role in the life cycle of the virus and has long been a target in antiviral therapy. Resistance of HIV protease to protease inhibitors (PIs) is problematic for the effective treatment of HIV infection. The South African HIV-1 subtype C protease (C-SA PR), which contains eight polymorphisms relative to the consensus HIV-1 subtype B protease, was expressed in Escherichia coli, purified, and crystallized. The crystal structure of the C-SA PR was resolved at 2.7?Å, which is the first crystal structure of a HIV-1 subtype C protease that predominates in Africa. Structural analyses of the C-SA PR in comparison to HIV-1 subtype B proteases indicated that polymorphisms at position 36 of the homodimeric HIV-1 protease may impact on the stability of the hinge region of the protease, and hence the dynamics of the flap region. Molecular dynamics simulations showed that the flap region of the C-SA PR displays a wider range of movements over time as compared to the subtype B proteases. Reduced stability in the hinge region resulting from the absent E35-R57 salt bridge in the C-SA PR, most likely contributes to the increased flexibility of the flaps which may be associated with reduced susceptibility to PIs.

An animated interactive 3D complement (I3DC) is available in Proteopedia at http://proteopedia.org/w/Journal:JBSD:36     

Cooperative fluctuations of unliganded and substrate-bound HIV-1 protease: a structure-based analysis on a variety of conformations from crystallography and molecular dynamics simulations

The dynamics of HIV-1 protease, both in unliganded and substrate-bound forms have been analyzed by using an analytical method, Gaussian network model (GNM). The method is applied to different conformations accessible to the protein backbone in the native state, observed in crystal structures and snapshots from fully atomistic molecular dynamics (MD) simulation trajectories. The modes of motion obtained from GNM on different conformations of HIV-1 protease are conserved throughout the MD simulations. The flaps and 40's loop of the unliganded HIV-1 protease structure are identified as the most mobile regions. However, in the liganded structure these flaps lose mobility, and terminal regions of the monomers become more flexible. Analysis of the fast modes shows that residues important for stability are in the same regions of all the structures examined. Among these, Gly86 appears to be a key residue for stability. The contribution of residues in the active site region and flaps to the stability is more pronounced in the substrate-bound form than in the unliganded form. The convergence of modes in GNM to similar regions of HIV-1 protease, regardless of the conformation of the protein, supports the robustness of GNM as a potentially useful and predictive tool.     

Atomistic simulations of the HIV-1 protease folding inhibition

Biochemical experiments have recently revealed that the p-S8 peptide, with an amino-acid sequence identical to the conserved fragment 83-93 (S8) of the HIV-1 protease, can inhibit catalytic activity of the enzyme by interfering with protease folding and dimerization. In this study, we introduce a hierarchical modeling approach for understanding the molecular basis of the HIV-1 protease folding inhibition. Coarse-grained molecular docking simulations of the flexible p-S8 peptide with the ensembles of HIV-1 protease monomers have revealed structurally different complexes of the p-S8 peptide, which can be formed by targeting the conserved segment 24-34 (S2) of the folding nucleus (folding inhibition) and by interacting with the antiparallel termini β-sheet region (dimerization inhibition). All-atom molecular dynamics simulations of the inhibitor complexes with the HIV-1 PR monomer have been independently carried out for the predicted folding and dimerization binding modes of the p-S8 peptide, confirming the thermodynamic stability of these complexes. Binding free-energy calculations of the p-S8 peptide and its active analogs are then performed using molecular dynamics trajectories of the peptide complexes with the HIV-1 PR monomers. The results of this study have provided a plausible molecular model for the inhibitor intervention with the HIV-1 PR folding and dimerization and have accurately reproduced the experimental inhibition profiles of the active folding inhibitors.     

Structure and dynamics of human vimentin intermediate filament dimer and tetramer in explicit and implicit solvent models

Intermediate filaments, in addition to microtubules and microfilaments, are one of the three major components of the cytoskeleton in eukaryotic cells, and play an important role in mechanotransduction as well as in providing mechanical stability to cells at large stretch. The molecular structures, mechanical and dynamical properties of the intermediate filament basic building blocks, the dimer and the tetramer, however, have remained elusive due to persistent experimental challenges owing to the large size and fibrillar geometry of this protein. We have recently reported an atomistic-level model of the human vimentin dimer and tetramer, obtained through a bottom-up approach based on structural optimization via molecular simulation based on an implicit solvent model (Qin et al. in PLoS ONE 2009 4(10):e7294, 9). Here we present extensive simulations and structural analyses of the model based on ultra large-scale atomistic-level simulations in an explicit solvent model, with system sizes exceeding 500,000 atoms and simulations carried out at 20 ns time-scales. We report a detailed comparison of the structural and dynamical behavior of this large biomolecular model with implicit and explicit solvent models. Our simulations confirm the stability of the molecular model and provide insight into the dynamical properties of the dimer and tetramer. Specifically, our simulations reveal a heterogeneous distribution of the bending stiffness along the molecular axis with the formation of rather soft and highly flexible hinge-like regions defined by non-alpha-helical linker domains. We report a comparison of Ramachandran maps and the solvent accessible surface area between implicit and explicit solvent models, and compute the persistence length of the dimer and tetramer structure of vimentin intermediate filaments for various subdomains of the protein. Our simulations provide detailed insight into the dynamical properties of the vimentin dimer and tetramer intermediate filament building blocks, which may guide the development of novel coarse-grained models of intermediate filaments, and could also help in understanding assembly mechanisms.     

Protein Structure Prediction with a Combined Solvation Free Energy-Molecular Mechanics Force Field

Abstract

Models of protein structure are frequently used to determine the physical characteristics of a protein when the crystal structure is not available. We developed a procedure to optimize such models, by use of a combined solvation free energy and molecular mechanics force field. Appropriately chosen atomic solvation parameters were defined using the criterion that the resulting protein model should deviate least from the crystal structure upon a forty picosecond molecular dynamics simulation carried out using the combined force field. Several tests were performed to refine the set of atomic solvation parameters which best complement the molecular mechanics forces. Four sets of parameters from the literature were tested and an empirically optimized set is proposed. The parameters are defined on a well characterized small molecule (alanyl dipeptide) and on the highly refined crystal structure of rat trypsin, and then tested on a second highly refined crystal structure of α-lytic protease. The new set of atomic solvation parameters provides a significant improvement over molecular mechanics alone in energy minimization of protein structures. This combined force field also has advantages over the use of explicit solvent as it is possible to take solvent effects into account during energetic conformational searching when modeling a homologous protein structure from a known crystal structure.     

Molecular dynamics effects on protein electrostatics

Electrostatic calculations have been carried out on a number of structural conformers of tuna cytochrome c. Conformers were generated using molecular dynamics simulations with a range of solvent simulating, macroscopic dielectric formalisms, and one solvent model that explicitly included solvent water molecules. Structures generated using the lowest dielectric models were relatively tight, with side chains collapsed on the surface, while those from the higher dielectric models had more internal and external fluidity, with surface side chains exploring a fuller range of conformational space. The average structure generated with the explicitly solvated model corresponded most closely with the crystal structure. Individual pK values, overall titration curves, and electrostatic potential surfaces were calculated for average structures and structures along each simulation. Differences between structural conformers within each simulation give rise to substantial changes in calculated local electrostatic interactions, resulting in pK value fluctuations for individual sites in the protein that vary by 0.3-2.0 pK units from the calculated time average. These variations are due to the thermal side chain reorientations that produce fluctuations in charge site separations. Properties like overall titration curves and pH dependent stability are not as sensitive to side chain fluctuations within a simulation, but there are substantial effects between simulations due to marked differences in average side chain behavior. These findings underscore the importance of proper dielectric formalism in molecular dynamics simulations when used to generate alternate solution structures from a crystal structure, and suggest that conformers significantly removed from the average structure have altered electrostatic properties that may prove important in episodic protein properties such as catalysis.     

Molecular dynamics simulation of trp-aporepressor in a solvent.

Molecular dynamics simulations of Escherichia coli trp-aporepressor were carried out in the absence and presence of explicit water molecules. The vacuum simulations resulted in significant deformation of the initial X-ray structure. A solvated simulation with a nonbonded cut-off radius of 9 A gave a better result, and the most satisfactory result was obtained when electrostatic interactions within a cut-off radius of 18 A were considered by a twin-range method. The trajectory from the last simulation was used to analyze the dynamical properties of the aporepressor. The root-mean-square fluctuations of the residues showed the rigidity of the central core and the flexibility of the DNA-binding sites, consistent with the X-ray temperature factors. The dynamical cross-correlation map indicated a significant negative correlation between the central core and the two DNA-binding sites, and thus reproduced the three-domain format (a central core and two DNA-binding heads) from a dynamical point of view. The core region showed weak, but many, intra- and inter-molecular correlations, while the helix-turn-helix DNA-binding motifs were free from correlations with other regions.     

Electrostatic screening in molecular dynamics simulations.

The screened Coulombic potential has been shown to describe satisfactorily equilibrium properties like pK shifts, the effects of charged groups on redox potentials and binding constants of metal ions. To test how well the screening of the electrostatic potential describes the dynamical trajectory of a macromolecular system, a series of comparative simulations have been carried out on a protein system which explicitly included water molecules and a system in vacuo. For the system without solvent the results of using (i) the standard potential form were compared with results of (ii) the potential where the Coulomb term was modified by the inclusion of a distance dependent dielectric, epsilon (r), to model the screening effect of bulk water, and (iii) standard potential modified by reducing the charge on ionized residue side chains. All molecular dynamics simulations have been carried out on bovine pancreatic trypsin inhibitor. Comparisons between the resulting trajectories, averaged structures, hydrogen bonding patterns and properties such as solvent accessible surface area and radius of gyration are described. The results show that the dynamical behaviour of the protein calculated with a screened electrostatic term compares more favourably with the time-dependent structural changes of the full system with explicitly included water than the standard vacuum simulation.     

Conformational changes in HIV-1 proteinase: effect of protonation of the active center on conformation of HIV-1 proteinase in water

At weak acidic pH, where HIV-1 proteinase is most stable and active, its catalytic Asp 25/25' dyad shares one proton. At a physiological pH the dyad is deprotonated, however, 2 ns molecular dynamics simulations of the HIV-1 protease with monoprotonated and deprotonated Asp25/25' dyad is performed, in order to investigate the influence of Asp25/25' protonation state on the proteinase dynamics. For net charge neutralization the 4 Cl- ions were included. In case of deprotonated active site the significant tertiary structure deviation of HIV-1 PR structure from crystal structure is observed, while in the monoprotonated one the tertiary structure fluctuates near starting structure. Possible mechanism of the influence of the Asp25/25' protonation state on proteinase dynamics is discussed.     

Theoretical studies of relaxation of a monomeric subunit of HIV-1 protease in water using molecular dynamics

The dynamic behavior of one 99-residue subunit of the dimeric aspartyl protease of HIV-1 was studied in a 160 psec molecular dynamics simulation at 300 K in water. The crystal structure of one of the identical subunits of the dimer was the starting point, with the aqueous phase modeled by 4,331 explicit waters in a restrained spherical droplet Analysis of the simulations showed that the monomer displayed considerable flexibility in the interfacial portions of the flap (the region which folds over the substrate), the N- and C-0termini, and, to a lesser extent, the active site. The flap undergoes significant motion as an independent rigid finger, but without the cantilever previously reported hi a simulation of the dimer. The N-terminus displayed the greatest fluctuational disorder whereas the C-terminus exhibited the greatest root mean square movement from the crystal structure. The central core of the monomer had a heavy-atom root mean square deviation from the initial structure of about 3.0 Å during the latter half of the simulation. Although this is larger than the 1.6 Å found for comparable simulations of typical globular proteins, the general features of the tertiary structure were preserved over the course of the simulation. Overall, these results indicate that the relaxed structure obtained in these simulations may provide a better model for the tertiary structure of the solvated HIV-1 protease monomer than the subunit conformation seen in the X-ray crystallographic structure of the dimer. Except in the flap region, the design of compounds intended to interfere with dimerization should take this relaxation and the flexibility of the solvated monomer, especially at the termini, into account. © 1993 Wiley-Liss, Inc.     

A diverse view of protein dynamics from NMR studies of HIV-1 protease flaps

Internal motion in proteins fulfills a multitude of roles in biological processes. NMR spectroscopy has been applied to elucidate protein dynamics at the atomic level, albeit at a low resolution, and is often complemented by molecular dynamics simulation. However, it is critical to justify the consistency between simulation results and conclusions often drawn from multiple experiments in which uncertainties arising from assumed motional models may not be explicitly evaluated. To understand the role of the flaps of HIV-1 protease dimer in substrate recognition and protease function, many molecular dynamics simulations have been performed. The simulations have resulted in various proposed models of the flap dynamics, some of which are more consistent than others with our working model previously derived from experiments. However, using the working model to discriminate among the simulation results is not straightforward because the working model was derived from a combination of NMR experiments and crystal structure data. In this study, we use the NMR chemical shifts and relaxation data of the protease "monomer" rather than structural data to narrow down the possible conformations of the flaps of the "dimer". For the first time, we show that the tips of the flaps in the unliganded protease dimer interact with each other in solution. Accordingly, we discuss the consistency of the simulations with the model derived from all experimental data.     

Molecular dynamics studies on HIV-1 protease: a comparison of the flap motions between wild type protease and the M46I/G51D double mutant

The emergence of drug-resistant mutants of HIV-1 is a tragic effect associated with conventional long-treatment therapies against acquired immunodeficiency syndrome. These mutations frequently involve the aspartic protease encoded by the virus; knowledge of the molecular mechanisms underlying the conformational changes of HIV-1 protease mutants may be useful in developing more effective and longer lasting treatment regimes. The flap regions of the protease are the target of a particular type of mutations occurring far from the active site. These mutations modify the affinity for both substrate and ligands, thus conferring resistance. In this work, molecular dynamics simulations were performed on a native wild type HIV-1 protease and on the drug-resistant M46I/G51D double mutant. The simulation was carried out for a time of 3.5 ns using the GROMOS96 force field, with implementation of the SPC216 explicit solvation model. The results show that the flaps may exist in an ensemble of conformations between a “closed” and an “open” conformation. The behaviour of the flap tips during simulations is different between the native enzyme and the mutant. The mutation pattern leads to stabilization of the flaps in a semi-open configuration.     

High resolution crystal structures of HIV-1 protease with a potent non-peptide inhibitor (UIC-94017) active against multi-drug-resistant clinical strains

The compound UIC-94017 (TMC-114) is a second-generation HIV protease inhibitor with improved pharmacokinetics that is chemically related to the clinical inhibitor amprenavir. UIC-94017 is a broad-spectrum potent inhibitor active against HIV-1 clinical isolates with minimal cytotoxicity. We have determined the high-resolution crystal structures of UIC-94017 in complexes with wild-type HIV-1 protease (PR) and mutant proteases PR(V82A) and PR(I84V) that are common in drug-resistant HIV. The structures were refined at resolutions of 1.10-1.53A. The crystal structures of PR and PR(I84V) with UIC-94017 ternary complexes show that the inhibitor binds to the protease in two overlapping positions, while the PR(V82A) complex had one ordered inhibitor. In all three structures, UIC-94017 forms hydrogen bonds with the conserved main-chain atoms of Asp29 and Asp30 of the protease. These interactions are proposed to be critical for the potency of this compound against HIV isolates that are resistant to multiple protease inhibitors. Other small differences were observed in the interactions of the mutants with UIC-94017 as compared to PR. PR(V82A) showed differences in the position of the main-chain atoms of residue 82 compared to PR structure that better accommodated the inhibitor. Finally, the 1.10A resolution structure of PR(V82A) with UIC-94017 showed an unusual distribution of electron density for the catalytic aspartate residues, which is discussed in relation to the reaction mechanism.     

Cell killing by HIV-1 protease

The human immunodeficiency virus protease (HIV-1 PR) was expressed both in the yeast Saccharomyces cerevisiae and in mammalian cells. Inducible expression of HIV-1 PR arrested yeast growth, which was followed by cell lysis. The lytic phenotype included loss of plasma membrane integrity and cell wall breakage leading to the release of cell content to the medium. Given that neither poliovirus 2A protease nor 2BC protein, both being highly toxic for S. cerevisiae, were able to produce similar effects, it seems that this lytic phenotype is specific of HIV-1 PR. Drastic alterations in membrane permeability preceded the lysis in yeast expressing HIV-1 PR. Cell killing and lysis provoked by HIV-1 PR were also observed in mammalian cells. Thus, COS7 cells expressing the protease showed increased plasma membrane permeability and underwent lysis by necrosis with no signs of apoptosis. Strikingly, the morphological alterations induced by HIV-1 PR in yeast and mammalian cells were similar in many aspects. To our knowledge, this is the first report of a viral protein with such an activity. These findings contribute to the present knowledge on HIV-1-induced cytopathogenesis.     

Molecular dynamics simulations of bovine rhodopsin: influence of protonation states and different membrane-mimicking environments

G-protein coupled receptors (GPCRs) are a protein family of outstanding pharmaceutical interest. GPCR homology models, based on the crystal structure of bovine rhodopsin, have been shown to be valuable tools in the drug-design process. The initial model is often refined by molecular dynamics (MD) simulations, a procedure that has been recently discussed controversially. We therefore analyzed MD simulations of bovine rhodopsin in order to identify contacts that could serve as constraints in the simulation of homology models. Additionally, the effect of an N-terminal truncation, the nature of the membrane mimic, the influence of varying protonation states of buried residues and the importance of internal water molecules was analyzed. All simulations were carried out using the program-package GROMACS. While N-terminal truncation negatively influenced the overall protein stability, a stable simulation was possible in both solvent environments. As regards the protonation state of titratable sites, the experimental data could be reproduced by the program UHBD (University of Houston Brownian Dynamics), suggesting its application for studying homology models of GPCRs. A high flexibility was observed for internal water molecules at some sites. Finally, interhelical hydrogen-bonding interactions could be derived, which can now serve as constraints in the simulations of GPCR homology models.     

The folding and dimerization of HIV-1 protease: evidence for a stable monomer from simulations

HIV-1 protease (PR) is a major drug target in combating AIDS, as it plays a key role in maturation and replication of the virus. Six FDA-approved drugs are currently in clinical use, all designed to inhibit enzyme activity by blocking the active site, which exists only in the dimer. An alternative inhibition mode would be required to overcome the emergence of drug-resistance through the accumulation of mutations. This might involve inhibiting the formation of the dimer itself. Here, the folding of HIV-1 PR dimer is studied with several simulation models appropriate for folding mechanism studies. Simulations with an off-lattice Gō-model, which corresponds to a perfectly funneled energy landscape, indicate that the enzyme is formed by association of structured monomers. All-atom molecular dynamics simulations strongly support the stability of an isolated monomer. The conjunction of results from a model that focuses on the protein topology and a detailed all-atom force-field model suggests, in contradiction to some reported equilibrium denaturation experiments, that monomer folding and dimerization are decoupled. The simulation result is, however, in agreement with the recent NMR detection of folded monomers of HIV-1 PR mutants with a destabilized interface. Accordingly, the design of dimerization inhibitors should not focus only on the flexible N and C termini that constitute most of the dimer interface, but also on other structured regions of the monomer. In particular, the relatively high phi values for residues 23-35 and 79-87 in both the folding and binding transition states, together with their proximity to the interface, highlight them as good targets for inhibitor design.